1 | MODULE limthd |
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2 | !!====================================================================== |
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3 | !! *** MODULE limthd *** |
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4 | !! LIM-3 : ice thermodynamic |
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5 | !!====================================================================== |
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6 | !! History : LIM ! 2000-01 (M.A. Morales Maqueda, H. Goosse, T. Fichefet) LIM-1 |
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7 | !! 2.0 ! 2002-07 (C. Ethe, G. Madec) LIM-2 (F90 rewriting) |
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8 | !! 3.0 ! 2005-11 (M. Vancoppenolle) LIM-3 : Multi-layer thermodynamics + salinity variations |
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9 | !! - ! 2007-04 (M. Vancoppenolle) add lim_thd_glohec, lim_thd_con_dh and lim_thd_con_dif |
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10 | !! 3.2 ! 2009-07 (M. Vancoppenolle, Y. Aksenov, G. Madec) bug correction in rdmsnif |
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11 | !! 3.3 ! 2010-11 (G. Madec) corrected snow melting heat (due to factor betas) |
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12 | !! 4.0 ! 2011-02 (G. Madec) dynamical allocation |
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13 | !!---------------------------------------------------------------------- |
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14 | #if defined key_lim3 |
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15 | !!---------------------------------------------------------------------- |
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16 | !! 'key_lim3' LIM3 sea-ice model |
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17 | !!---------------------------------------------------------------------- |
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18 | !! lim_thd : thermodynamic of sea ice |
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19 | !! lim_thd_init : initialisation of sea-ice thermodynamic |
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20 | !!---------------------------------------------------------------------- |
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21 | USE phycst ! physical constants |
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22 | USE dom_oce ! ocean space and time domain variables |
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23 | USE ice ! LIM: sea-ice variables |
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24 | USE par_ice ! LIM: sea-ice parameters |
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25 | USE sbc_oce ! Surface boundary condition: ocean fields |
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26 | USE sbc_ice ! Surface boundary condition: ice fields |
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27 | USE thd_ice ! LIM thermodynamic sea-ice variables |
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28 | USE dom_ice ! LIM sea-ice domain |
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29 | USE domvvl ! domain: variable volume level |
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30 | USE limthd_dif ! LIM: thermodynamics, vertical diffusion |
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31 | USE limthd_dh ! LIM: thermodynamics, ice and snow thickness variation |
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32 | USE limthd_sal ! LIM: thermodynamics, ice salinity |
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33 | USE limthd_ent ! LIM: thermodynamics, ice enthalpy redistribution |
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34 | USE limtab ! LIM: 1D <==> 2D transformation |
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35 | USE limvar ! LIM: sea-ice variables |
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36 | USE lbclnk ! lateral boundary condition - MPP links |
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37 | USE lib_mpp ! MPP library |
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38 | USE in_out_manager ! I/O manager |
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39 | USE prtctl ! Print control |
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40 | |
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41 | IMPLICIT NONE |
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42 | PRIVATE |
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43 | |
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44 | PUBLIC lim_thd ! called by limstp module |
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45 | PUBLIC lim_thd_init ! called by iceini module |
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46 | |
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47 | REAL(wp) :: epsi20 = 1e-20_wp ! constant values |
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48 | REAL(wp) :: epsi16 = 1e-16_wp ! |
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49 | REAL(wp) :: epsi10 = 1e-10_wp ! |
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50 | REAL(wp) :: epsi06 = 1e-06_wp ! |
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51 | REAL(wp) :: epsi04 = 1e-04_wp ! |
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52 | REAL(wp) :: zzero = 0._wp ! |
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53 | REAL(wp) :: zone = 1._wp ! |
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54 | |
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55 | !! * Substitutions |
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56 | # include "domzgr_substitute.h90" |
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57 | # include "vectopt_loop_substitute.h90" |
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58 | !!---------------------------------------------------------------------- |
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59 | !! NEMO/LIM3 3.3 , UCL - NEMO Consortium (2010) |
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60 | !! $Id$ |
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61 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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62 | !!---------------------------------------------------------------------- |
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63 | CONTAINS |
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64 | |
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65 | SUBROUTINE lim_thd( kt ) |
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66 | !!------------------------------------------------------------------- |
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67 | !! *** ROUTINE lim_thd *** |
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68 | !! |
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69 | !! ** Purpose : This routine manages the ice thermodynamic. |
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70 | !! |
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71 | !! ** Action : - Initialisation of some variables |
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72 | !! - Some preliminary computation (oceanic heat flux |
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73 | !! at the ice base, snow acc.,heat budget of the leads) |
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74 | !! - selection of the icy points and put them in an array |
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75 | !! - call lim_vert_ther for vert ice thermodynamic |
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76 | !! - back to the geographic grid |
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77 | !! - selection of points for lateral accretion |
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78 | !! - call lim_lat_acc for the ice accretion |
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79 | !! - back to the geographic grid |
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80 | !! |
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81 | !! ** References : H. Goosse et al. 1996, Bul. Soc. Roy. Sc. Liege, 65, 87-90 |
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82 | !!--------------------------------------------------------------------- |
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83 | USE wrk_nemo, ONLY: wrk_in_use, wrk_not_released |
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84 | USE wrk_nemo, ONLY: zqlbsbq => wrk_2d_1 ! 2D workspace |
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85 | ! |
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86 | INTEGER, INTENT(in) :: kt ! number of iteration |
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87 | !! |
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88 | INTEGER :: ji, jj, jk, jl ! dummy loop indices |
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89 | INTEGER :: nbpb ! nb of icy pts for thermo. cal. |
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90 | REAL(wp) :: zfric_umin = 5e-03_wp ! lower bound for the friction velocity |
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91 | REAL(wp) :: zfric_umax = 2e-02_wp ! upper bound for the friction velocity |
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92 | REAL(wp) :: zinda, zindb, zthsnice, zfric_u ! local scalar |
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93 | REAL(wp) :: zfntlat, zpareff, zareamin, zcoef ! - - |
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94 | !!------------------------------------------------------------------- |
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95 | |
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96 | IF( wrk_in_use(2, 1) ) THEN |
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97 | CALL ctl_stop( 'lim_thd : requested workspace arrays unavailable' ) ; RETURN |
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98 | ENDIF |
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99 | |
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100 | !------------------------------------------------------------------------------! |
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101 | ! 1) Initialization of diagnostic variables ! |
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102 | !------------------------------------------------------------------------------! |
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103 | |
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104 | !-------------------- |
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105 | ! 1.2) Heat content |
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106 | !-------------------- |
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107 | ! Change the units of heat content; from global units to J.m3 |
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108 | DO jl = 1, jpl |
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109 | DO jk = 1, nlay_i |
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110 | DO jj = 1, jpj |
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111 | DO ji = 1, jpi |
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112 | !Energy of melting q(S,T) [J.m-3] |
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113 | e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_i(ji,jj,jl) , epsi06 ) ) * nlay_i |
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114 | !0 if no ice and 1 if yes |
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115 | zindb = 1.0 - MAX ( 0.0 , SIGN ( 1.0 , - ht_i(ji,jj,jl) ) ) |
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116 | !convert units ! very important that this line is here |
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117 | e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) * unit_fac * zindb |
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118 | END DO |
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119 | END DO |
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120 | END DO |
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121 | DO jk = 1, nlay_s |
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122 | DO jj = 1, jpj |
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123 | DO ji = 1, jpi |
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124 | !Energy of melting q(S,T) [J.m-3] |
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125 | e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_s(ji,jj,jl) , epsi06 ) ) * nlay_s |
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126 | !0 if no ice and 1 if yes |
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127 | zindb = 1.0 - MAX ( 0.0 , SIGN ( 1.0 , - ht_s(ji,jj,jl) ) ) |
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128 | !convert units ! very important that this line is here |
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129 | e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) * unit_fac * zindb |
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130 | END DO |
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131 | END DO |
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132 | END DO |
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133 | END DO |
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134 | |
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135 | !----------------------------- |
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136 | ! 1.3) Set some dummies to 0 |
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137 | !----------------------------- |
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138 | rdvosif(:,:) = 0.e0 ! variation of ice volume at surface |
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139 | rdvobif(:,:) = 0.e0 ! variation of ice volume at bottom |
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140 | fdvolif(:,:) = 0.e0 ! total variation of ice volume |
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141 | rdvonif(:,:) = 0.e0 ! lateral variation of ice volume |
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142 | fstric (:,:) = 0.e0 ! part of solar radiation transmitted through the ice |
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143 | ffltbif(:,:) = 0.e0 ! linked with fstric |
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144 | qfvbq (:,:) = 0.e0 ! linked with fstric |
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145 | rdmsnif(:,:) = 0.e0 ! variation of snow mass per unit area |
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146 | rdmicif(:,:) = 0.e0 ! variation of ice mass per unit area |
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147 | hicifp (:,:) = 0.e0 ! daily thermodynamic ice production. |
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148 | fsbri (:,:) = 0.e0 ! brine flux contribution to salt flux to the ocean |
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149 | fhbri (:,:) = 0.e0 ! brine flux contribution to heat flux to the ocean |
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150 | fseqv (:,:) = 0.e0 ! equivalent salt flux to the ocean due to ice/growth decay |
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151 | |
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152 | !----------------------------------- |
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153 | ! 1.4) Compute global heat content |
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154 | !----------------------------------- |
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155 | qt_i_in (:,:) = 0.e0 |
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156 | qt_s_in (:,:) = 0.e0 |
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157 | qt_i_fin (:,:) = 0.e0 |
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158 | qt_s_fin (:,:) = 0.e0 |
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159 | sum_fluxq(:,:) = 0.e0 |
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160 | fatm (:,:) = 0.e0 |
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161 | |
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162 | ! 2) Partial computation of forcing for the thermodynamic sea ice model. ! |
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163 | !-----------------------------------------------------------------------------! |
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164 | |
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165 | !CDIR NOVERRCHK |
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166 | DO jj = 1, jpj |
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167 | !CDIR NOVERRCHK |
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168 | DO ji = 1, jpi |
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169 | zthsnice = SUM( ht_s(ji,jj,1:jpl) ) + SUM( ht_i(ji,jj,1:jpl) ) |
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170 | zindb = tms(ji,jj) * ( 1.0 - MAX( zzero , SIGN( zone , - zthsnice ) ) ) |
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171 | phicif(ji,jj) = vt_i(ji,jj) |
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172 | pfrld(ji,jj) = 1.0 - at_i(ji,jj) |
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173 | zinda = 1.0 - MAX( zzero , SIGN( zone , - ( 1.0 - pfrld(ji,jj) ) ) ) |
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174 | ! |
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175 | ! ! solar irradiance transmission at the mixed layer bottom and used in the lead heat budget |
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176 | ! ! practically no "direct lateral ablation" |
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177 | ! |
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178 | ! ! net downward heat flux from the ice to the ocean, expressed as a function of ocean |
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179 | ! ! temperature and turbulent mixing (McPhee, 1992) |
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180 | ! friction velocity |
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181 | zfric_u = MAX ( MIN( SQRT( ust2s(ji,jj) ) , zfric_umax ) , zfric_umin ) |
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182 | |
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183 | ! here the drag will depend on ice thickness and type (0.006) |
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184 | fdtcn(ji,jj) = zindb * rau0 * rcp * 0.006 * zfric_u * ( (sst_m(ji,jj) + rt0) - t_bo(ji,jj) ) |
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185 | ! also category dependent |
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186 | ! !-- Energy from the turbulent oceanic heat flux heat flux coming in the lead |
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187 | qdtcn(ji,jj) = zindb * fdtcn(ji,jj) * (1.0 - at_i(ji,jj)) * rdt_ice |
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188 | ! |
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189 | ! !-- Lead heat budget, qldif (part 1, next one is in limthd_dh) |
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190 | ! ! caution: exponent betas used as more snow can fallinto leads |
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191 | qldif(ji,jj) = tms(ji,jj) * rdt_ice * ( & |
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192 | & pfrld(ji,jj) * ( qsr(ji,jj) & ! solar heat |
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193 | & + qns(ji,jj) & ! non solar heat |
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194 | & + fdtcn(ji,jj) & ! turbulent ice-ocean heat |
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195 | & + fsbbq(ji,jj) * ( 1.0 - zindb ) ) & ! residual heat from previous step |
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196 | & - pfrld(ji,jj)**betas * sprecip(ji,jj) * lfus ) ! latent heat of sprecip melting |
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197 | ! |
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198 | ! Positive heat budget is used for bottom ablation |
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199 | zfntlat = 1.0 - MAX( zzero , SIGN( zone , - qldif(ji,jj) ) ) |
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200 | != 1 if positive heat budget |
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201 | zpareff = 1.0 - zinda * zfntlat |
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202 | != 0 if ice and positive heat budget and 1 if one of those two is false |
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203 | zqlbsbq(ji,jj) = qldif(ji,jj) * ( 1.0 - zpareff ) / MAX( at_i(ji,jj) * rdt_ice , epsi16 ) |
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204 | ! |
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205 | ! Heat budget of the lead, energy transferred from ice to ocean |
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206 | qldif (ji,jj) = zpareff * qldif(ji,jj) |
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207 | qdtcn (ji,jj) = zpareff * qdtcn(ji,jj) |
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208 | ! |
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209 | ! Energy needed to bring ocean surface layer until its freezing (qcmif, limflx) |
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210 | qcmif (ji,jj) = rau0 * rcp * fse3t(ji,jj,1) * ( t_bo(ji,jj) - (sst_m(ji,jj) + rt0) ) * ( 1. - zinda ) |
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211 | ! |
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212 | ! oceanic heat flux (limthd_dh) |
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213 | fbif (ji,jj) = zindb * ( fsbbq(ji,jj) / MAX( at_i(ji,jj) , epsi20 ) + fdtcn(ji,jj) ) |
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214 | ! |
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215 | END DO |
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216 | END DO |
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217 | |
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218 | !------------------------------------------------------------------------------! |
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219 | ! 3) Select icy points and fulfill arrays for the vectorial grid. |
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220 | !------------------------------------------------------------------------------! |
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221 | |
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222 | DO jl = 1, jpl !loop over ice categories |
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223 | |
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224 | IF( kt == nit000 .AND. lwp ) THEN |
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225 | WRITE(numout,*) ' lim_thd : transfer to 1D vectors. Category no : ', jl |
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226 | WRITE(numout,*) ' ~~~~~~~~' |
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227 | ENDIF |
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228 | |
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229 | zareamin = 1.e-10 |
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230 | nbpb = 0 |
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231 | DO jj = 1, jpj |
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232 | DO ji = 1, jpi |
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233 | IF ( a_i(ji,jj,jl) .gt. zareamin ) THEN |
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234 | nbpb = nbpb + 1 |
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235 | npb(nbpb) = (jj - 1) * jpi + ji |
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236 | ENDIF |
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237 | ! debug point to follow |
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238 | IF ( (ji.eq.jiindx).AND.(jj.eq.jjindx) ) THEN |
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239 | jiindex_1d = nbpb |
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240 | ENDIF |
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241 | END DO |
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242 | END DO |
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243 | |
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244 | !------------------------------------------------------------------------------! |
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245 | ! 4) Thermodynamic computation |
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246 | !------------------------------------------------------------------------------! |
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247 | |
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248 | IF( lk_mpp ) CALL mpp_ini_ice( nbpb , numout ) |
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249 | |
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250 | IF( nbpb > 0 ) THEN ! If there is no ice, do nothing. |
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251 | |
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252 | !------------------------- |
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253 | ! 4.1 Move to 1D arrays |
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254 | !------------------------- |
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255 | |
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256 | CALL tab_2d_1d( nbpb, at_i_b (1:nbpb), at_i , jpi, jpj, npb(1:nbpb) ) |
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257 | CALL tab_2d_1d( nbpb, a_i_b (1:nbpb), a_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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258 | CALL tab_2d_1d( nbpb, ht_i_b (1:nbpb), ht_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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259 | CALL tab_2d_1d( nbpb, ht_s_b (1:nbpb), ht_s(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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260 | |
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261 | CALL tab_2d_1d( nbpb, t_su_b (1:nbpb), t_su(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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262 | CALL tab_2d_1d( nbpb, sm_i_b (1:nbpb), sm_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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263 | DO jk = 1, nlay_s |
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264 | CALL tab_2d_1d( nbpb, t_s_b(1:nbpb,jk), t_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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265 | CALL tab_2d_1d( nbpb, q_s_b(1:nbpb,jk), e_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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266 | END DO |
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267 | DO jk = 1, nlay_i |
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268 | CALL tab_2d_1d( nbpb, t_i_b(1:nbpb,jk), t_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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269 | CALL tab_2d_1d( nbpb, q_i_b(1:nbpb,jk), e_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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270 | CALL tab_2d_1d( nbpb, s_i_b(1:nbpb,jk), s_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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271 | END DO |
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272 | |
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273 | CALL tab_2d_1d( nbpb, tatm_ice_1d(1:nbpb), tatm_ice(:,:) , jpi, jpj, npb(1:nbpb) ) |
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274 | CALL tab_2d_1d( nbpb, qsr_ice_1d (1:nbpb), qsr_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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275 | CALL tab_2d_1d( nbpb, fr1_i0_1d (1:nbpb), fr1_i0 , jpi, jpj, npb(1:nbpb) ) |
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276 | CALL tab_2d_1d( nbpb, fr2_i0_1d (1:nbpb), fr2_i0 , jpi, jpj, npb(1:nbpb) ) |
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277 | CALL tab_2d_1d( nbpb, qnsr_ice_1d(1:nbpb), qns_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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278 | |
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279 | #if ! defined key_coupled |
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280 | CALL tab_2d_1d( nbpb, qla_ice_1d (1:nbpb), qla_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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281 | CALL tab_2d_1d( nbpb, dqla_ice_1d(1:nbpb), dqla_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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282 | #endif |
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283 | |
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284 | CALL tab_2d_1d( nbpb, dqns_ice_1d(1:nbpb), dqns_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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285 | CALL tab_2d_1d( nbpb, t_bo_b (1:nbpb), t_bo , jpi, jpj, npb(1:nbpb) ) |
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286 | CALL tab_2d_1d( nbpb, sprecip_1d (1:nbpb), sprecip , jpi, jpj, npb(1:nbpb) ) |
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287 | CALL tab_2d_1d( nbpb, fbif_1d (1:nbpb), fbif , jpi, jpj, npb(1:nbpb) ) |
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288 | CALL tab_2d_1d( nbpb, qldif_1d (1:nbpb), qldif , jpi, jpj, npb(1:nbpb) ) |
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289 | CALL tab_2d_1d( nbpb, rdmicif_1d (1:nbpb), rdmicif , jpi, jpj, npb(1:nbpb) ) |
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290 | CALL tab_2d_1d( nbpb, rdmsnif_1d (1:nbpb), rdmsnif , jpi, jpj, npb(1:nbpb) ) |
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291 | CALL tab_2d_1d( nbpb, dmgwi_1d (1:nbpb), dmgwi , jpi, jpj, npb(1:nbpb) ) |
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292 | CALL tab_2d_1d( nbpb, qlbbq_1d (1:nbpb), zqlbsbq , jpi, jpj, npb(1:nbpb) ) |
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293 | |
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294 | CALL tab_2d_1d( nbpb, fseqv_1d (1:nbpb), fseqv , jpi, jpj, npb(1:nbpb) ) |
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295 | CALL tab_2d_1d( nbpb, fsbri_1d (1:nbpb), fsbri , jpi, jpj, npb(1:nbpb) ) |
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296 | CALL tab_2d_1d( nbpb, fhbri_1d (1:nbpb), fhbri , jpi, jpj, npb(1:nbpb) ) |
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297 | CALL tab_2d_1d( nbpb, fstbif_1d (1:nbpb), fstric , jpi, jpj, npb(1:nbpb) ) |
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298 | CALL tab_2d_1d( nbpb, qfvbq_1d (1:nbpb), qfvbq , jpi, jpj, npb(1:nbpb) ) |
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299 | |
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300 | !-------------------------------- |
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301 | ! 4.3) Thermodynamic processes |
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302 | !-------------------------------- |
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303 | |
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304 | IF( con_i ) CALL lim_thd_enmelt( 1, nbpb ) ! computes sea ice energy of melting |
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305 | IF( con_i ) CALL lim_thd_glohec( qt_i_in, qt_s_in, q_i_layer_in, 1, nbpb, jl ) |
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306 | |
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307 | ! !---------------------------------! |
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308 | CALL lim_thd_dif( 1, nbpb, jl ) ! Ice/Snow Temperature profile ! |
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309 | ! !---------------------------------! |
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310 | |
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311 | CALL lim_thd_enmelt( 1, nbpb ) ! computes sea ice energy of melting compulsory for limthd_dh |
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312 | |
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313 | IF( con_i ) CALL lim_thd_glohec ( qt_i_fin, qt_s_fin, q_i_layer_fin, 1, nbpb, jl ) |
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314 | IF( con_i ) CALL lim_thd_con_dif( 1 , nbpb , jl ) |
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315 | |
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316 | ! !---------------------------------! |
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317 | CALL lim_thd_dh( 1, nbpb, jl ) ! Ice/Snow thickness ! |
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318 | ! !---------------------------------! |
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319 | |
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320 | ! !---------------------------------! |
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321 | CALL lim_thd_ent( 1, nbpb, jl ) ! Ice/Snow enthalpy remapping ! |
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322 | ! !---------------------------------! |
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323 | |
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324 | ! !---------------------------------! |
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325 | CALL lim_thd_sal( 1, nbpb ) ! Ice salinity computation ! |
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326 | ! !---------------------------------! |
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327 | |
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328 | ! CALL lim_thd_enmelt(1,nbpb) ! computes sea ice energy of melting |
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329 | IF( con_i ) CALL lim_thd_glohec( qt_i_fin, qt_s_fin, q_i_layer_fin, 1, nbpb, jl ) |
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330 | IF( con_i ) CALL lim_thd_con_dh ( 1 , nbpb , jl ) |
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331 | |
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332 | !-------------------------------- |
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333 | ! 4.4) Move 1D to 2D vectors |
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334 | !-------------------------------- |
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335 | |
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336 | CALL tab_1d_2d( nbpb, at_i , npb, at_i_b(1:nbpb), jpi, jpj ) |
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337 | CALL tab_1d_2d( nbpb, ht_i(:,:,jl), npb, ht_i_b(1:nbpb), jpi, jpj ) |
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338 | CALL tab_1d_2d( nbpb, ht_s(:,:,jl), npb, ht_s_b(1:nbpb), jpi, jpj ) |
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339 | CALL tab_1d_2d( nbpb, a_i (:,:,jl), npb, a_i_b(1:nbpb) , jpi, jpj ) |
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340 | CALL tab_1d_2d( nbpb, t_su(:,:,jl), npb, t_su_b(1:nbpb), jpi, jpj ) |
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341 | CALL tab_1d_2d( nbpb, sm_i(:,:,jl), npb, sm_i_b(1:nbpb), jpi, jpj ) |
---|
342 | |
---|
343 | DO jk = 1, nlay_s |
---|
344 | CALL tab_1d_2d( nbpb, t_s(:,:,jk,jl), npb, t_s_b(1:nbpb,jk), jpi, jpj) |
---|
345 | CALL tab_1d_2d( nbpb, e_s(:,:,jk,jl), npb, q_s_b(1:nbpb,jk), jpi, jpj) |
---|
346 | END DO |
---|
347 | |
---|
348 | DO jk = 1, nlay_i |
---|
349 | CALL tab_1d_2d( nbpb, t_i(:,:,jk,jl), npb, t_i_b(1:nbpb,jk), jpi, jpj) |
---|
350 | CALL tab_1d_2d( nbpb, e_i(:,:,jk,jl), npb, q_i_b(1:nbpb,jk), jpi, jpj) |
---|
351 | CALL tab_1d_2d( nbpb, s_i(:,:,jk,jl), npb, s_i_b(1:nbpb,jk), jpi, jpj) |
---|
352 | END DO |
---|
353 | |
---|
354 | CALL tab_1d_2d( nbpb, fstric , npb, fstbif_1d (1:nbpb), jpi, jpj ) |
---|
355 | CALL tab_1d_2d( nbpb, qldif , npb, qldif_1d (1:nbpb), jpi, jpj ) |
---|
356 | CALL tab_1d_2d( nbpb, qfvbq , npb, qfvbq_1d (1:nbpb), jpi, jpj ) |
---|
357 | CALL tab_1d_2d( nbpb, rdmicif, npb, rdmicif_1d(1:nbpb), jpi, jpj ) |
---|
358 | CALL tab_1d_2d( nbpb, rdmsnif, npb, rdmsnif_1d(1:nbpb), jpi, jpj ) |
---|
359 | CALL tab_1d_2d( nbpb, dmgwi , npb, dmgwi_1d (1:nbpb), jpi, jpj ) |
---|
360 | CALL tab_1d_2d( nbpb, rdvosif, npb, dvsbq_1d (1:nbpb), jpi, jpj ) |
---|
361 | CALL tab_1d_2d( nbpb, rdvobif, npb, dvbbq_1d (1:nbpb), jpi, jpj ) |
---|
362 | CALL tab_1d_2d( nbpb, fdvolif, npb, dvlbq_1d (1:nbpb), jpi, jpj ) |
---|
363 | CALL tab_1d_2d( nbpb, rdvonif, npb, dvnbq_1d (1:nbpb), jpi, jpj ) |
---|
364 | CALL tab_1d_2d( nbpb, fseqv , npb, fseqv_1d (1:nbpb), jpi, jpj ) |
---|
365 | ! |
---|
366 | IF( num_sal == 2 ) THEN |
---|
367 | CALL tab_1d_2d( nbpb, fsbri, npb, fsbri_1d(1:nbpb), jpi, jpj ) |
---|
368 | CALL tab_1d_2d( nbpb, fhbri, npb, fhbri_1d(1:nbpb), jpi, jpj ) |
---|
369 | ENDIF |
---|
370 | ! |
---|
371 | !+++++ |
---|
372 | !temporary stuff for a dummy version |
---|
373 | CALL tab_1d_2d( nbpb, dh_i_surf2D, npb, dh_i_surf(1:nbpb) , jpi, jpj ) |
---|
374 | CALL tab_1d_2d( nbpb, dh_i_bott2D, npb, dh_i_bott(1:nbpb) , jpi, jpj ) |
---|
375 | CALL tab_1d_2d( nbpb, fsup2D , npb, fsup (1:nbpb) , jpi, jpj ) |
---|
376 | CALL tab_1d_2d( nbpb, focea2D , npb, focea (1:nbpb) , jpi, jpj ) |
---|
377 | CALL tab_1d_2d( nbpb, s_i_newice , npb, s_i_new (1:nbpb) , jpi, jpj ) |
---|
378 | CALL tab_1d_2d( nbpb, izero(:,:,jl) , npb, i0 (1:nbpb) , jpi, jpj ) |
---|
379 | CALL tab_1d_2d( nbpb, qns_ice(:,:,jl), npb, qnsr_ice_1d(1:nbpb), jpi, jpj) |
---|
380 | !+++++ |
---|
381 | ! |
---|
382 | IF( lk_mpp ) CALL mpp_comm_free( ncomm_ice ) !RB necessary ?? |
---|
383 | ENDIF |
---|
384 | ! |
---|
385 | END DO |
---|
386 | |
---|
387 | !------------------------------------------------------------------------------! |
---|
388 | ! 5) Global variables, diagnostics |
---|
389 | !------------------------------------------------------------------------------! |
---|
390 | |
---|
391 | !------------------------ |
---|
392 | ! 5.1) Ice heat content |
---|
393 | !------------------------ |
---|
394 | ! Enthalpies are global variables we have to readjust the units |
---|
395 | zcoef = 1._wp / ( unit_fac * REAL( nlay_i ) ) |
---|
396 | DO jl = 1, jpl |
---|
397 | DO jk = 1, nlay_i |
---|
398 | ! Multiply by volume, divide by nlayers so that heat content in 10^9 Joules |
---|
399 | e_i(:,:,jk,jl) = e_i(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_i(:,:,jl) * zcoef |
---|
400 | END DO |
---|
401 | END DO |
---|
402 | |
---|
403 | !------------------------ |
---|
404 | ! 5.2) Snow heat content |
---|
405 | !------------------------ |
---|
406 | ! Enthalpies are global variables we have to readjust the units |
---|
407 | zcoef = 1._wp / ( unit_fac * REAL( nlay_s ) ) |
---|
408 | DO jl = 1, jpl |
---|
409 | DO jk = 1, nlay_s |
---|
410 | ! Multiply by volume, so that heat content in 10^9 Joules |
---|
411 | e_s(:,:,jk,jl) = e_s(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_s(:,:,jl) * zcoef |
---|
412 | END DO |
---|
413 | END DO |
---|
414 | |
---|
415 | !---------------------------------- |
---|
416 | ! 5.3) Change thickness to volume |
---|
417 | !---------------------------------- |
---|
418 | CALL lim_var_eqv2glo |
---|
419 | |
---|
420 | !-------------------------------------------- |
---|
421 | ! 5.4) Diagnostic thermodynamic growth rates |
---|
422 | !-------------------------------------------- |
---|
423 | d_v_i_thd(:,:,:) = v_i (:,:,:) - old_v_i(:,:,:) ! ice volumes |
---|
424 | dv_dt_thd(:,:,:) = d_v_i_thd(:,:,:) / rdt_ice * 86400.0 |
---|
425 | |
---|
426 | IF( con_i ) fbif(:,:) = fbif(:,:) + zqlbsbq(:,:) |
---|
427 | |
---|
428 | IF(ln_ctl) THEN ! Control print |
---|
429 | CALL prt_ctl_info(' ') |
---|
430 | CALL prt_ctl_info(' - Cell values : ') |
---|
431 | CALL prt_ctl_info(' ~~~~~~~~~~~~~ ') |
---|
432 | CALL prt_ctl(tab2d_1=area , clinfo1=' lim_thd : cell area :') |
---|
433 | CALL prt_ctl(tab2d_1=at_i , clinfo1=' lim_thd : at_i :') |
---|
434 | CALL prt_ctl(tab2d_1=vt_i , clinfo1=' lim_thd : vt_i :') |
---|
435 | CALL prt_ctl(tab2d_1=vt_s , clinfo1=' lim_thd : vt_s :') |
---|
436 | DO jl = 1, jpl |
---|
437 | CALL prt_ctl_info(' ') |
---|
438 | CALL prt_ctl_info(' - Category : ', ivar1=jl) |
---|
439 | CALL prt_ctl_info(' ~~~~~~~~~~') |
---|
440 | CALL prt_ctl(tab2d_1=a_i (:,:,jl) , clinfo1= ' lim_thd : a_i : ') |
---|
441 | CALL prt_ctl(tab2d_1=ht_i (:,:,jl) , clinfo1= ' lim_thd : ht_i : ') |
---|
442 | CALL prt_ctl(tab2d_1=ht_s (:,:,jl) , clinfo1= ' lim_thd : ht_s : ') |
---|
443 | CALL prt_ctl(tab2d_1=v_i (:,:,jl) , clinfo1= ' lim_thd : v_i : ') |
---|
444 | CALL prt_ctl(tab2d_1=v_s (:,:,jl) , clinfo1= ' lim_thd : v_s : ') |
---|
445 | CALL prt_ctl(tab2d_1=e_s (:,:,1,jl) , clinfo1= ' lim_thd : e_s : ') |
---|
446 | CALL prt_ctl(tab2d_1=t_su (:,:,jl) , clinfo1= ' lim_thd : t_su : ') |
---|
447 | CALL prt_ctl(tab2d_1=t_s (:,:,1,jl) , clinfo1= ' lim_thd : t_snow : ') |
---|
448 | CALL prt_ctl(tab2d_1=sm_i (:,:,jl) , clinfo1= ' lim_thd : sm_i : ') |
---|
449 | CALL prt_ctl(tab2d_1=smv_i (:,:,jl) , clinfo1= ' lim_thd : smv_i : ') |
---|
450 | DO jk = 1, nlay_i |
---|
451 | CALL prt_ctl_info(' ') |
---|
452 | CALL prt_ctl_info(' - Layer : ', ivar1=jk) |
---|
453 | CALL prt_ctl_info(' ~~~~~~~') |
---|
454 | CALL prt_ctl(tab2d_1=t_i(:,:,jk,jl) , clinfo1= ' lim_thd : t_i : ') |
---|
455 | CALL prt_ctl(tab2d_1=e_i(:,:,jk,jl) , clinfo1= ' lim_thd : e_i : ') |
---|
456 | END DO |
---|
457 | END DO |
---|
458 | ENDIF |
---|
459 | ! |
---|
460 | IF( wrk_not_released(2, 1) ) CALL ctl_stop( 'lim_thd: failed to release workspace arrays' ) |
---|
461 | ! |
---|
462 | END SUBROUTINE lim_thd |
---|
463 | |
---|
464 | |
---|
465 | SUBROUTINE lim_thd_glohec( eti, ets, etilayer, kideb, kiut, jl ) |
---|
466 | !!----------------------------------------------------------------------- |
---|
467 | !! *** ROUTINE lim_thd_glohec *** |
---|
468 | !! |
---|
469 | !! ** Purpose : Compute total heat content for each category |
---|
470 | !! Works with 1d vectors only |
---|
471 | !!----------------------------------------------------------------------- |
---|
472 | INTEGER , INTENT(in ) :: kideb, kiut ! bounds for the spatial loop |
---|
473 | INTEGER , INTENT(in ) :: jl ! category number |
---|
474 | REAL(wp), INTENT( out), DIMENSION (jpij,jpl ) :: eti, ets ! vertically-summed heat content for ice & snow |
---|
475 | REAL(wp), INTENT( out), DIMENSION (jpij,jkmax) :: etilayer ! heat content for ice layers |
---|
476 | !! |
---|
477 | INTEGER :: ji,jk ! loop indices |
---|
478 | !!----------------------------------------------------------------------- |
---|
479 | eti(:,:) = 0._wp |
---|
480 | ets(:,:) = 0._wp |
---|
481 | ! |
---|
482 | DO jk = 1, nlay_i ! total q over all layers, ice [J.m-2] |
---|
483 | DO ji = kideb, kiut |
---|
484 | etilayer(ji,jk) = q_i_b(ji,jk) * ht_i_b(ji) / nlay_i |
---|
485 | eti (ji,jl) = eti(ji,jl) + etilayer(ji,jk) |
---|
486 | END DO |
---|
487 | END DO |
---|
488 | DO ji = kideb, kiut ! total q over all layers, snow [J.m-2] |
---|
489 | ets(ji,jl) = ets(ji,jl) + q_s_b(ji,1) * ht_s_b(ji) / nlay_s |
---|
490 | END DO |
---|
491 | ! |
---|
492 | IF(lwp) WRITE(numout,*) ' lim_thd_glohec ' |
---|
493 | IF(lwp) WRITE(numout,*) ' qt_i_in : ', eti(jiindex_1d,jl) / rdt_ice |
---|
494 | IF(lwp) WRITE(numout,*) ' qt_s_in : ', ets(jiindex_1d,jl) / rdt_ice |
---|
495 | IF(lwp) WRITE(numout,*) ' qt_in : ', ( eti(jiindex_1d,jl) + ets(jiindex_1d,jl) ) / rdt_ice |
---|
496 | ! |
---|
497 | END SUBROUTINE lim_thd_glohec |
---|
498 | |
---|
499 | |
---|
500 | SUBROUTINE lim_thd_con_dif( kideb, kiut, jl ) |
---|
501 | !!----------------------------------------------------------------------- |
---|
502 | !! *** ROUTINE lim_thd_con_dif *** |
---|
503 | !! |
---|
504 | !! ** Purpose : Test energy conservation after heat diffusion |
---|
505 | !!------------------------------------------------------------------- |
---|
506 | INTEGER , INTENT(in ) :: kideb, kiut ! bounds for the spatial loop |
---|
507 | INTEGER , INTENT(in ) :: jl ! category number |
---|
508 | |
---|
509 | INTEGER :: ji, jk ! loop indices |
---|
510 | INTEGER :: zji, zjj |
---|
511 | INTEGER :: numce ! number of points for which conservation is violated |
---|
512 | REAL(wp) :: meance ! mean conservation error |
---|
513 | REAL(wp) :: max_cons_err, max_surf_err |
---|
514 | !!--------------------------------------------------------------------- |
---|
515 | |
---|
516 | max_cons_err = 1.0_wp ! maximum tolerated conservation error |
---|
517 | max_surf_err = 0.001_wp ! maximum tolerated surface error |
---|
518 | |
---|
519 | !-------------------------- |
---|
520 | ! Increment of energy |
---|
521 | !-------------------------- |
---|
522 | ! global |
---|
523 | DO ji = kideb, kiut |
---|
524 | dq_i(ji,jl) = qt_i_fin(ji,jl) - qt_i_in(ji,jl) + qt_s_fin(ji,jl) - qt_s_in(ji,jl) |
---|
525 | END DO |
---|
526 | ! layer by layer |
---|
527 | dq_i_layer(:,:) = q_i_layer_fin(:,:) - q_i_layer_in(:,:) |
---|
528 | |
---|
529 | !---------------------------------------- |
---|
530 | ! Atmospheric heat flux, ice heat budget |
---|
531 | !---------------------------------------- |
---|
532 | DO ji = kideb, kiut |
---|
533 | zji = MOD( npb(ji) - 1 , jpi ) + 1 |
---|
534 | zjj = ( npb(ji) - 1 ) / jpi + 1 |
---|
535 | fatm (ji,jl) = qnsr_ice_1d(ji) + ( 1._wp - i0(ji) ) * qsr_ice_1d(ji) |
---|
536 | sum_fluxq(ji,jl) = fc_su(ji) - fc_bo_i(ji) + qsr_ice_1d(ji) * i0(ji) - fstroc(zji,zjj,jl) |
---|
537 | END DO |
---|
538 | |
---|
539 | !-------------------- |
---|
540 | ! Conservation error |
---|
541 | !-------------------- |
---|
542 | DO ji = kideb, kiut |
---|
543 | cons_error(ji,jl) = ABS( dq_i(ji,jl) / rdt_ice + sum_fluxq(ji,jl) ) |
---|
544 | END DO |
---|
545 | |
---|
546 | numce = 0 |
---|
547 | meance = 0._wp |
---|
548 | DO ji = kideb, kiut |
---|
549 | IF ( cons_error(ji,jl) .GT. max_cons_err ) THEN |
---|
550 | numce = numce + 1 |
---|
551 | meance = meance + cons_error(ji,jl) |
---|
552 | ENDIF |
---|
553 | END DO |
---|
554 | IF( numce > 0 ) meance = meance / numce |
---|
555 | |
---|
556 | WRITE(numout,*) ' Maximum tolerated conservation error : ', max_cons_err |
---|
557 | WRITE(numout,*) ' After lim_thd_dif, category : ', jl |
---|
558 | WRITE(numout,*) ' Mean conservation error on big error points ', meance, numit |
---|
559 | WRITE(numout,*) ' Number of points where there is a cons err gt than c.e. : ', numce, numit |
---|
560 | |
---|
561 | !------------------------------------------------------- |
---|
562 | ! Surface error due to imbalance between Fatm and Fcsu |
---|
563 | !------------------------------------------------------- |
---|
564 | numce = 0 |
---|
565 | meance = 0._wp |
---|
566 | |
---|
567 | DO ji = kideb, kiut |
---|
568 | surf_error(ji,jl) = ABS ( fatm(ji,jl) - fc_su(ji) ) |
---|
569 | IF( ( t_su_b(ji) .LT. rtt ) .AND. ( surf_error(ji,jl) .GT. max_surf_err ) ) THEN |
---|
570 | numce = numce + 1 |
---|
571 | meance = meance + surf_error(ji,jl) |
---|
572 | ENDIF |
---|
573 | ENDDO |
---|
574 | IF( numce > 0 ) meance = meance / numce |
---|
575 | |
---|
576 | WRITE(numout,*) ' Maximum tolerated surface error : ', max_surf_err |
---|
577 | WRITE(numout,*) ' After lim_thd_dif, category : ', jl |
---|
578 | WRITE(numout,*) ' Mean surface error on big error points ', meance, numit |
---|
579 | WRITE(numout,*) ' Number of points where there is a surf err gt than surf_err : ', numce, numit |
---|
580 | |
---|
581 | IF (jiindex_1D.GT.0) WRITE(numout,*) ' fc_su : ', fc_su(jiindex_1d) |
---|
582 | IF (jiindex_1D.GT.0) WRITE(numout,*) ' fatm : ', fatm(jiindex_1d,jl) |
---|
583 | IF (jiindex_1D.GT.0) WRITE(numout,*) ' t_su : ', t_su_b(jiindex_1d) |
---|
584 | |
---|
585 | !--------------------------------------- |
---|
586 | ! Write ice state in case of big errors |
---|
587 | !--------------------------------------- |
---|
588 | DO ji = kideb, kiut |
---|
589 | IF ( ( ( t_su_b(ji) .LT. rtt ) .AND. ( surf_error(ji,jl) .GT. max_surf_err ) ) .OR. & |
---|
590 | ( cons_error(ji,jl) .GT. max_cons_err ) ) THEN |
---|
591 | zji = MOD( npb(ji) - 1, jpi ) + 1 |
---|
592 | zjj = ( npb(ji) - 1 ) / jpi + 1 |
---|
593 | ! |
---|
594 | WRITE(numout,*) ' alerte 1 ' |
---|
595 | WRITE(numout,*) ' Untolerated conservation / surface error after ' |
---|
596 | WRITE(numout,*) ' heat diffusion in the ice ' |
---|
597 | WRITE(numout,*) ' Category : ', jl |
---|
598 | WRITE(numout,*) ' zji , zjj : ', zji, zjj |
---|
599 | WRITE(numout,*) ' lat, lon : ', gphit(zji,zjj), glamt(zji,zjj) |
---|
600 | WRITE(numout,*) ' cons_error : ', cons_error(ji,jl) |
---|
601 | WRITE(numout,*) ' surf_error : ', surf_error(ji,jl) |
---|
602 | WRITE(numout,*) ' dq_i : ', - dq_i(ji,jl) / rdt_ice |
---|
603 | WRITE(numout,*) ' Fdt : ', sum_fluxq(ji,jl) |
---|
604 | WRITE(numout,*) |
---|
605 | ! WRITE(numout,*) ' qt_i_in : ', qt_i_in(ji,jl) |
---|
606 | ! WRITE(numout,*) ' qt_s_in : ', qt_s_in(ji,jl) |
---|
607 | ! WRITE(numout,*) ' qt_i_fin : ', qt_i_fin(ji,jl) |
---|
608 | ! WRITE(numout,*) ' qt_s_fin : ', qt_s_fin(ji,jl) |
---|
609 | ! WRITE(numout,*) ' qt : ', qt_i_fin(ji,jl) + qt_s_fin(ji,jl) |
---|
610 | WRITE(numout,*) ' ht_i : ', ht_i_b(ji) |
---|
611 | WRITE(numout,*) ' ht_s : ', ht_s_b(ji) |
---|
612 | WRITE(numout,*) ' t_su : ', t_su_b(ji) |
---|
613 | WRITE(numout,*) ' t_s : ', t_s_b(ji,1) |
---|
614 | WRITE(numout,*) ' t_i : ', t_i_b(ji,1:nlay_i) |
---|
615 | WRITE(numout,*) ' t_bo : ', t_bo_b(ji) |
---|
616 | WRITE(numout,*) ' q_i : ', q_i_b(ji,1:nlay_i) |
---|
617 | WRITE(numout,*) ' s_i : ', s_i_b(ji,1:nlay_i) |
---|
618 | WRITE(numout,*) ' tmelts : ', rtt - tmut*s_i_b(ji,1:nlay_i) |
---|
619 | WRITE(numout,*) |
---|
620 | WRITE(numout,*) ' Fluxes ' |
---|
621 | WRITE(numout,*) ' ~~~~~~ ' |
---|
622 | WRITE(numout,*) ' fatm : ', fatm(ji,jl) |
---|
623 | WRITE(numout,*) ' fc_su : ', fc_su (ji) |
---|
624 | WRITE(numout,*) ' fstr_inice : ', qsr_ice_1d(ji)*i0(ji) |
---|
625 | WRITE(numout,*) ' fc_bo : ', - fc_bo_i (ji) |
---|
626 | WRITE(numout,*) ' foc : ', fbif_1d(ji) |
---|
627 | WRITE(numout,*) ' fstroc : ', fstroc (zji,zjj,jl) |
---|
628 | WRITE(numout,*) ' i0 : ', i0(ji) |
---|
629 | WRITE(numout,*) ' qsr_ice : ', (1.0-i0(ji))*qsr_ice_1d(ji) |
---|
630 | WRITE(numout,*) ' qns_ice : ', qnsr_ice_1d(ji) |
---|
631 | WRITE(numout,*) ' Conduction fluxes : ' |
---|
632 | WRITE(numout,*) ' fc_s : ', fc_s(ji,0:nlay_s) |
---|
633 | WRITE(numout,*) ' fc_i : ', fc_i(ji,0:nlay_i) |
---|
634 | WRITE(numout,*) |
---|
635 | WRITE(numout,*) ' Layer by layer ... ' |
---|
636 | WRITE(numout,*) ' dq_snow : ', ( qt_s_fin(ji,jl) - qt_s_in(ji,jl) ) / rdt_ice |
---|
637 | WRITE(numout,*) ' dfc_snow : ', fc_s(ji,1) - fc_s(ji,0) |
---|
638 | DO jk = 1, nlay_i |
---|
639 | WRITE(numout,*) ' layer : ', jk |
---|
640 | WRITE(numout,*) ' dq_ice : ', dq_i_layer(ji,jk) / rdt_ice |
---|
641 | WRITE(numout,*) ' radab : ', radab(ji,jk) |
---|
642 | WRITE(numout,*) ' dfc_i : ', fc_i(ji,jk) - fc_i(ji,jk-1) |
---|
643 | WRITE(numout,*) ' tot f : ', fc_i(ji,jk) - fc_i(ji,jk-1) - radab(ji,jk) |
---|
644 | END DO |
---|
645 | |
---|
646 | ENDIF |
---|
647 | ! |
---|
648 | END DO |
---|
649 | ! |
---|
650 | END SUBROUTINE lim_thd_con_dif |
---|
651 | |
---|
652 | |
---|
653 | SUBROUTINE lim_thd_con_dh( kideb, kiut, jl ) |
---|
654 | !!----------------------------------------------------------------------- |
---|
655 | !! *** ROUTINE lim_thd_con_dh *** |
---|
656 | !! |
---|
657 | !! ** Purpose : Test energy conservation after enthalpy redistr. |
---|
658 | !!----------------------------------------------------------------------- |
---|
659 | INTEGER, INTENT(in) :: kideb, kiut ! bounds for the spatial loop |
---|
660 | INTEGER, INTENT(in) :: jl ! category number |
---|
661 | ! |
---|
662 | INTEGER :: ji ! loop indices |
---|
663 | INTEGER :: zji, zjj, numce ! local integers |
---|
664 | REAL(wp) :: meance, max_cons_err !local scalar |
---|
665 | !!--------------------------------------------------------------------- |
---|
666 | |
---|
667 | max_cons_err = 1._wp |
---|
668 | |
---|
669 | !-------------------------- |
---|
670 | ! Increment of energy |
---|
671 | !-------------------------- |
---|
672 | DO ji = kideb, kiut |
---|
673 | dq_i(ji,jl) = qt_i_fin(ji,jl) - qt_i_in(ji,jl) + qt_s_fin(ji,jl) - qt_s_in(ji,jl) ! global |
---|
674 | END DO |
---|
675 | dq_i_layer(:,:) = q_i_layer_fin(:,:) - q_i_layer_in(:,:) ! layer by layer |
---|
676 | |
---|
677 | !---------------------------------------- |
---|
678 | ! Atmospheric heat flux, ice heat budget |
---|
679 | !---------------------------------------- |
---|
680 | DO ji = kideb, kiut |
---|
681 | zji = MOD( npb(ji) - 1 , jpi ) + 1 |
---|
682 | zjj = ( npb(ji) - 1 ) / jpi + 1 |
---|
683 | |
---|
684 | fatm (ji,jl) = qnsr_ice_1d(ji) + qsr_ice_1d(ji) ! total heat flux |
---|
685 | sum_fluxq (ji,jl) = fatm(ji,jl) + fbif_1d(ji) - ftotal_fin(ji) - fstroc(zji,zjj,jl) |
---|
686 | cons_error(ji,jl) = ABS( dq_i(ji,jl) / rdt_ice + sum_fluxq(ji,jl) ) |
---|
687 | END DO |
---|
688 | |
---|
689 | !-------------------- |
---|
690 | ! Conservation error |
---|
691 | !-------------------- |
---|
692 | DO ji = kideb, kiut |
---|
693 | cons_error(ji,jl) = ABS( dq_i(ji,jl) / rdt_ice + sum_fluxq(ji,jl) ) |
---|
694 | END DO |
---|
695 | |
---|
696 | numce = 0 |
---|
697 | meance = 0._wp |
---|
698 | DO ji = kideb, kiut |
---|
699 | IF( cons_error(ji,jl) .GT. max_cons_err ) THEN |
---|
700 | numce = numce + 1 |
---|
701 | meance = meance + cons_error(ji,jl) |
---|
702 | ENDIF |
---|
703 | ENDDO |
---|
704 | IF(numce > 0 ) meance = meance / numce |
---|
705 | |
---|
706 | WRITE(numout,*) ' Error report - Category : ', jl |
---|
707 | WRITE(numout,*) ' ~~~~~~~~~~~~ ' |
---|
708 | WRITE(numout,*) ' Maximum tolerated conservation error : ', max_cons_err |
---|
709 | WRITE(numout,*) ' After lim_thd_ent, category : ', jl |
---|
710 | WRITE(numout,*) ' Mean conservation error on big error points ', meance, numit |
---|
711 | WRITE(numout,*) ' Number of points where there is a cons err gt than 0.1 W/m2 : ', numce, numit |
---|
712 | |
---|
713 | !--------------------------------------- |
---|
714 | ! Write ice state in case of big errors |
---|
715 | !--------------------------------------- |
---|
716 | DO ji = kideb, kiut |
---|
717 | IF ( cons_error(ji,jl) .GT. max_cons_err ) THEN |
---|
718 | zji = MOD( npb(ji) - 1, jpi ) + 1 |
---|
719 | zjj = ( npb(ji) - 1 ) / jpi + 1 |
---|
720 | ! |
---|
721 | WRITE(numout,*) ' alerte 1 - category : ', jl |
---|
722 | WRITE(numout,*) ' Untolerated conservation error after limthd_ent ' |
---|
723 | WRITE(numout,*) ' zji , zjj : ', zji, zjj |
---|
724 | WRITE(numout,*) ' lat, lon : ', gphit(zji,zjj), glamt(zji,zjj) |
---|
725 | WRITE(numout,*) ' * ' |
---|
726 | WRITE(numout,*) ' Ftotal : ', sum_fluxq(ji,jl) |
---|
727 | WRITE(numout,*) ' dq_t : ', - dq_i(ji,jl) / rdt_ice |
---|
728 | WRITE(numout,*) ' dq_i : ', - ( qt_i_fin(ji,jl) - qt_i_in(ji,jl) ) / rdt_ice |
---|
729 | WRITE(numout,*) ' dq_s : ', - ( qt_s_fin(ji,jl) - qt_s_in(ji,jl) ) / rdt_ice |
---|
730 | WRITE(numout,*) ' cons_error : ', cons_error(ji,jl) |
---|
731 | WRITE(numout,*) ' * ' |
---|
732 | WRITE(numout,*) ' Fluxes --- : ' |
---|
733 | WRITE(numout,*) ' fatm : ', fatm(ji,jl) |
---|
734 | WRITE(numout,*) ' foce : ', fbif_1d(ji) |
---|
735 | WRITE(numout,*) ' fres : ', ftotal_fin(ji) |
---|
736 | WRITE(numout,*) ' fhbri : ', fhbricat(zji,zjj,jl) |
---|
737 | WRITE(numout,*) ' * ' |
---|
738 | WRITE(numout,*) ' Heat contents --- : ' |
---|
739 | WRITE(numout,*) ' qt_s_in : ', qt_s_in(ji,jl) / rdt_ice |
---|
740 | WRITE(numout,*) ' qt_i_in : ', qt_i_in(ji,jl) / rdt_ice |
---|
741 | WRITE(numout,*) ' qt_in : ', ( qt_i_in(ji,jl) + qt_s_in(ji,jl) ) / rdt_ice |
---|
742 | WRITE(numout,*) ' qt_s_fin : ', qt_s_fin(ji,jl) / rdt_ice |
---|
743 | WRITE(numout,*) ' qt_i_fin : ', qt_i_fin(ji,jl) / rdt_ice |
---|
744 | WRITE(numout,*) ' qt_fin : ', ( qt_i_fin(ji,jl) + qt_s_fin(ji,jl) ) / rdt_ice |
---|
745 | WRITE(numout,*) ' * ' |
---|
746 | WRITE(numout,*) ' Ice variables --- : ' |
---|
747 | WRITE(numout,*) ' ht_i : ', ht_i_b(ji) |
---|
748 | WRITE(numout,*) ' ht_s : ', ht_s_b(ji) |
---|
749 | WRITE(numout,*) ' dh_s_tot : ', dh_s_tot(ji) |
---|
750 | WRITE(numout,*) ' dh_snowice: ', dh_snowice(ji) |
---|
751 | WRITE(numout,*) ' dh_i_surf : ', dh_i_surf(ji) |
---|
752 | WRITE(numout,*) ' dh_i_bott : ', dh_i_bott(ji) |
---|
753 | ENDIF |
---|
754 | ! |
---|
755 | END DO |
---|
756 | ! |
---|
757 | END SUBROUTINE lim_thd_con_dh |
---|
758 | |
---|
759 | |
---|
760 | SUBROUTINE lim_thd_enmelt( kideb, kiut ) |
---|
761 | !!----------------------------------------------------------------------- |
---|
762 | !! *** ROUTINE lim_thd_enmelt *** |
---|
763 | !! |
---|
764 | !! ** Purpose : Computes sea ice energy of melting q_i (J.m-3) |
---|
765 | !! |
---|
766 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
---|
767 | !!------------------------------------------------------------------- |
---|
768 | INTEGER, INTENT(in) :: kideb, kiut ! bounds for the spatial loop |
---|
769 | !! |
---|
770 | INTEGER :: ji, jk ! dummy loop indices |
---|
771 | REAL(wp) :: ztmelts ! local scalar |
---|
772 | !!------------------------------------------------------------------- |
---|
773 | ! |
---|
774 | DO jk = 1, nlay_i ! Sea ice energy of melting |
---|
775 | DO ji = kideb, kiut |
---|
776 | ztmelts = - tmut * s_i_b(ji,jk) + rtt |
---|
777 | q_i_b(ji,jk) = rhoic * ( cpic * ( ztmelts - t_i_b(ji,jk) ) & |
---|
778 | & + lfus * ( 1.0 - (ztmelts-rtt) / MIN( t_i_b(ji,jk)-rtt, -epsi10 ) ) & |
---|
779 | & - rcp * ( ztmelts-rtt ) ) |
---|
780 | END DO |
---|
781 | END DO |
---|
782 | DO jk = 1, nlay_s ! Snow energy of melting |
---|
783 | DO ji = kideb, kiut |
---|
784 | q_s_b(ji,jk) = rhosn * ( cpic * ( rtt - t_s_b(ji,jk) ) + lfus ) |
---|
785 | END DO |
---|
786 | END DO |
---|
787 | ! |
---|
788 | END SUBROUTINE lim_thd_enmelt |
---|
789 | |
---|
790 | |
---|
791 | SUBROUTINE lim_thd_init |
---|
792 | !!----------------------------------------------------------------------- |
---|
793 | !! *** ROUTINE lim_thd_init *** |
---|
794 | !! |
---|
795 | !! ** Purpose : Physical constants and parameters linked to the ice |
---|
796 | !! thermodynamics |
---|
797 | !! |
---|
798 | !! ** Method : Read the namicethd namelist and check the ice-thermo |
---|
799 | !! parameter values called at the first timestep (nit000) |
---|
800 | !! |
---|
801 | !! ** input : Namelist namicether |
---|
802 | !!------------------------------------------------------------------- |
---|
803 | NAMELIST/namicethd/ hmelt , hiccrit, fraz_swi, maxfrazb, vfrazb, Cfrazb, & |
---|
804 | & hicmin, hiclim, amax , & |
---|
805 | & sbeta , parlat, hakspl, hibspl, exld, & |
---|
806 | & hakdif, hnzst , thth , parsub, alphs, betas, & |
---|
807 | & kappa_i, nconv_i_thd, maxer_i_thd, thcon_i_swi |
---|
808 | !!------------------------------------------------------------------- |
---|
809 | ! |
---|
810 | IF(lwp) THEN |
---|
811 | WRITE(numout,*) |
---|
812 | WRITE(numout,*) 'lim_thd : Ice Thermodynamics' |
---|
813 | WRITE(numout,*) '~~~~~~~' |
---|
814 | ENDIF |
---|
815 | ! |
---|
816 | REWIND( numnam_ice ) ! read Namelist numnam_ice |
---|
817 | READ ( numnam_ice , namicethd ) |
---|
818 | ! |
---|
819 | IF(lwp) THEN ! control print |
---|
820 | WRITE(numout,*) |
---|
821 | WRITE(numout,*)' Namelist of ice parameters for ice thermodynamic computation ' |
---|
822 | WRITE(numout,*)' maximum melting at the bottom hmelt = ', hmelt |
---|
823 | WRITE(numout,*)' ice thick. for lateral accretion in NH (SH) hiccrit(1/2) = ', hiccrit |
---|
824 | WRITE(numout,*)' Frazil ice thickness as a function of wind or not fraz_swi = ', fraz_swi |
---|
825 | WRITE(numout,*)' Maximum proportion of frazil ice collecting at bottom maxfrazb = ', maxfrazb |
---|
826 | WRITE(numout,*)' Thresold relative drift speed for collection of frazil vfrazb = ', vfrazb |
---|
827 | WRITE(numout,*)' Squeezing coefficient for collection of frazil Cfrazb = ', Cfrazb |
---|
828 | WRITE(numout,*)' ice thick. corr. to max. energy stored in brine pocket hicmin = ', hicmin |
---|
829 | WRITE(numout,*)' minimum ice thickness hiclim = ', hiclim |
---|
830 | WRITE(numout,*)' maximum lead fraction amax = ', amax |
---|
831 | WRITE(numout,*)' numerical carac. of the scheme for diffusion in ice ' |
---|
832 | WRITE(numout,*)' Cranck-Nicholson (=0.5), implicit (=1), explicit (=0) sbeta = ', sbeta |
---|
833 | WRITE(numout,*)' percentage of energy used for lateral ablation parlat = ', parlat |
---|
834 | WRITE(numout,*)' slope of distr. for Hakkinen-Mellor lateral melting hakspl = ', hakspl |
---|
835 | WRITE(numout,*)' slope of distribution for Hibler lateral melting hibspl = ', hibspl |
---|
836 | WRITE(numout,*)' exponent for leads-closure rate exld = ', exld |
---|
837 | WRITE(numout,*)' coefficient for diffusions of ice and snow hakdif = ', hakdif |
---|
838 | WRITE(numout,*)' threshold thick. for comp. of eq. thermal conductivity zhth = ', thth |
---|
839 | WRITE(numout,*)' thickness of the surf. layer in temp. computation hnzst = ', hnzst |
---|
840 | WRITE(numout,*)' switch for snow sublimation (=1) or not (=0) parsub = ', parsub |
---|
841 | WRITE(numout,*)' coefficient for snow density when snow ice formation alphs = ', alphs |
---|
842 | WRITE(numout,*)' coefficient for ice-lead partition of snowfall betas = ', betas |
---|
843 | WRITE(numout,*)' extinction radiation parameter in sea ice (1.0) kappa_i = ', kappa_i |
---|
844 | WRITE(numout,*)' maximal n. of iter. for heat diffusion computation nconv_i_thd = ', nconv_i_thd |
---|
845 | WRITE(numout,*)' maximal err. on T for heat diffusion computation maxer_i_thd = ', maxer_i_thd |
---|
846 | WRITE(numout,*)' switch for comp. of thermal conductivity in the ice thcon_i_swi = ', thcon_i_swi |
---|
847 | ENDIF |
---|
848 | ! |
---|
849 | rcdsn = hakdif * rcdsn |
---|
850 | rcdic = hakdif * rcdic |
---|
851 | ! |
---|
852 | END SUBROUTINE lim_thd_init |
---|
853 | |
---|
854 | #else |
---|
855 | !!---------------------------------------------------------------------- |
---|
856 | !! Default option Dummy module NO LIM3 sea-ice model |
---|
857 | !!---------------------------------------------------------------------- |
---|
858 | #endif |
---|
859 | |
---|
860 | !!====================================================================== |
---|
861 | END MODULE limthd |
---|